Ce掺杂TiO2/SiO2的制备及其光催化降解罗丹明B

采用溶胶-凝胶法制备了纯TiO2和掺杂不同含量Ce的TiO2/SiO2复合纳米粒子.并用FT-IR,UV-Vis对样品结构进行了表征,并以罗丹明B(RB)的光催化降解为探针反应,评价了其光催化性能.结果表明,TiO2/SiO2催化剂中形成了新的Ti-O-Si键,Ce的掺杂使TiC2/SiO2光谱响应范围向可见光区拓展.与未掺杂的TiO2/SiO2相比较,掺杂的TiO2/SiO2具有更高的催化性能.Ce掺杂的最佳值为x(Ce)∶x(Ti)=0.0090,光催化剂最佳投放量为30mg.     

Ce-TiO2光催化剂的制备与性能研究

采用溶胶-凝胶法制备了稀土Ce离子掺杂的纳米TiO2光催化剂(Ce-TiO2),通过XRD、FT-IR、UV-Vis、PL、Nano-sizer纳米粒度分析仪等对Ce-TiO2样品进行了表征和分析,并以亚甲基蓝(MB)作为目标降解物,考察了不同掺杂浓度及经不同温度热处理后的Ce-TiO2样品对MB的光催化降解效果,结果表明所制备样品的晶型均为锐钛矿相和金红石相的混晶相,Ce离子的掺杂拓展了TiO2在可见光区的光谱响应范围,提高了TiO2光催化活性。当pH值为1.5,Ce的掺杂量为n(Ce)∶n(TiO2)=1∶300,热处理温度为600℃条件下制备的样品其催化活性显著高于Degussa P25。     

羧甲基壳聚糖/Ce^3＋掺杂TiO2复合抗菌材料的研究

采用溶胶-凝胶法制备稀土（Ce^3＋）掺杂纳米TiO2（纳米Ce/TiO2）,借助XRD、BET、SEM对Ce/TiO2进行表征。结果表明纳米Ce/TiO2晶型为锐钛矿,平均晶粒大小为19.95nm,比表面积为43.302m^2/g。采用超声波催化法合成了羧甲基壳聚糖（CMC）,并与Ce/TiO2复配制得羧甲基壳聚糖/Ce3＋掺杂纳米TiO2复合材料（CMC/Ce/TiO2）,借助FT-IR对CMC及CMC/Ce/TiO2复合材料进行了结构表征。初步研究了纳米Ce/TiO2、普通纳米TiO2、CMC/Ce/TiO2、CMC的抗菌性能,结果显示纳米Ce/TiO2对大肠杆菌和金黄色葡萄球菌的抗菌率分别为55%和53%,普通纳米TiO2对两种菌的抗菌率分别为50%和45%,Ce^3＋的掺杂可提高纳米TiO2的抗菌性能;CMC/Ce/TiO2对大肠杆菌和金黄色葡萄球菌的抗菌率分别达到99%和95%,CMC对两种菌的抗菌率分别为90%和80%,Ce/TiO2的复合可显著提高CMC的抗菌性能。     

Ce/ZnO纳米复合抗菌剂的制备及其性能研究

以纳米氧化锌(ZnO)为载体,采用稀土离子掺杂的方法制备了Ce/ZnO纳米复合抗菌剂。通过TEM、XRD等技术对样品进行表征,结果表明:制备的Ce/ZnO复合粉体是一种纳米复合抗菌剂,粒径在20nm左右,并且铈以CeO2的化学态存在于Ce/ZnO复合粉体表面,在ZnO的位置上进行了有效掺杂。掺杂稀土铈有效的提高了纳米ZnO的光催化性能以及抗菌效果。     

铈掺杂TiO2/Ti光电极制备及可见光下光电催化性能的研究

采用阳极氧化法制备铈掺杂TiO2／Ti光电极，用SEM、XRD、XRF、XPS和UV／VIS／NIR对光电极的性能进行表征，并对其可见光照射下的光电催化性能进行了测试．研究结果表明：在成膜电压为160V，电流密度为100mA／cm^2，Ce（NO3）3浓度为960mg／L条件下制备的铈掺杂TiO2／Ti光电极在降解罗丹明B的实验中表现出良好的光电催化活性．     

金属离子掺杂TiO2的光催化性能研究

用醇盐水解法制备了Ce4+、Ag+、Fe3+、Fe2+、Sn4+、Zn2+、Mo6+等金属离子掺杂的TiO2复合微粒.以罗丹明6G降解为目标反应,研究了所制备的复合微粒光催化活性与选择性.并用IR、XRD、TEM及BET等技术,对TiO2复合微粒进行了表征.结果显示在TiO2内掺入Ce4+、Ag+、Sn4+,可使纳米TiO2的光催化活性增强,而Fe3+、Fe2+、Zn2+、Mo6+等金属离子掺杂的二氧化钛复合微粒的催化活性呈下降趋势.     

Fe_3O_4/Ce~(3+)-TiO_2复合光催化材料的制备及其光催化性能研究

采用溶胶-凝胶法,以钛酸四丁酯、硝酸铈为主要原料,无水乙醇为溶剂,冰醋酸为抑制剂,浓硝酸为催化剂制得稳定的Ce3+掺杂TiO2溶胶,其凝胶经不同温度煅烧3 h后制得Ce3+掺杂量不同的TiO2粉体。用XRD对TiO2进行了测试对比分析,以紫外光为光源,亚甲基蓝溶液为模拟有机染料废水,研究了TiO2的光催化性能。用化学共沉淀法制备了具有强磁性的纳米Fe3O4水基磁流体,再与Ce3+掺杂TiO2进行复合,制备了Fe3O4负载量不同的磁性Ce3+掺杂TiO2,研究了其对亚甲基蓝的光催化降解效果、磁分离回收率的影响。结果表明,TiO2凝胶热处理温度、Ce3+掺量、TiO2晶型及Fe3O4负载量对亚甲基蓝的光催化活性均有影响。掺Ce3+量为1%,热处理温度650℃的Ce3+掺杂TiO2粉体光催化活性最高。Fe3O4负载量为10%的Fe3O4/Ce3+-TiO2对亚甲基蓝的降解率8 h时达到90.3%,磁分离回收率达96.8%。     

镧铈混合掺杂TiO2纳米粉末的制备

用溶胶-凝胶法制备La和Ce混合掺杂的TiO2纳米粉.用透射电子显微镜(TEM)、X射线衍射(XRD)和X射线荧光光谱(XRF)对其进行表征.XRD数据显示合成的La和Ce共掺杂纳米TiO2粉末在480℃下煅烧6h样品均具有稳定的锐钛矿相.XRF数据显示了具体的掺杂含量.所制得的La和Ce混合掺杂纳米TiO2粉在电镜观...     

N掺杂TiO2纳米粉体的表面特性及可见光活性

旨在探究N掺杂纳米TiO2具有可见光活性的本质,采用XPS、ESR、XRD、SEM、DRS、SPS和PL分析技术对sol-gel法制备的未掺杂和N掺杂TiO2纳米粉体进行了对比研究,并以亚甲基蓝(MB)溶液在可见光下的光催化脱色评价其可见光活性。结果表明,N掺杂TiO2纳米粉体具有良好的可见光活性,未掺杂样品几乎没有可见光活性。N取代TiO2晶格中O形成了N─Ti─O和O─N─Ti键合结构产生杂质能级,N掺杂导致TiO2表面形成了大量束缚单电子的氧空位产生缺陷能级,二者协同作用致使带隙窄化,光吸收带边红移,产生可见光活性。N掺杂导致TiO2晶格中p-n结的形成及表面氧空位和表面羟基的增加均能促进光生e-/h+分离,有效抑制光生e-/h+复合,提高量子效率,进而提高其光活性。     

锌沸石-Ce/TiO2抗菌材料的制备及其性能研究

以纳米锐钛矿型TiO2粉体作为主要原料,锌沸石作为载体,铈离子为掺杂离子,采用浸渍法制备锌沸石-Ce/TiO2抗菌材料,运用抑菌圈法对其抗菌性能进行评价,用紫外光谱对比纯纳米TiO2抗菌材料和锌沸石-Ce/TiO2抗菌材料的光催化效果。结果表明,纳米TiO2与硝酸铈的物质的量比为40∶1、反应时间为0.5h、焙烧温度为300℃、pH=3条件下抗菌性能最佳,抑菌圈直径达到34.63mm。锌沸石-Ce/TiO2抗菌材料样品对于大肠杆菌具有明显的抑杀效果。     

Structural and optical properties of AlxOy/Pt/AlxOy multilayer absorber

We report on the microstructure and optical properties of Al_xO_y–Pt–Al_xO_y interference-type multilayer films, deposited by electron beam (e-beam) deposition onto corning 1737 glass, silicon (1 1 1) and copper substrates. The structural properties were investigated by Rutherford backscattering spectrometry, X-ray diffraction, scanning electron microscopy, energy dispersive X-ray spectroscopy and atomic force microscopy. The optical properties were extracted from specular reflection/transmission, diffuse reflectance and emissometer measurements. The stratification of the coatings consists of a semi-transparent middle Pt layer sandwiched between two layers of Al_xO_y. The top and bottom Al_xO_y layers were non-stoichiometric with no crystalline phases present. The Pt layer is in the fcc crystalline phase with a broad size distribution and spheroidal shape in and between the rims of Al_xO_y. The surface roughness of the stack was found to be comparable to the inter-particle distance. The optical calculations confirm a high solar absorptance of ∼0.94 and a low thermal emittance of ∼0.06 for the multilayer stack, which is attributed not only to the optimized nature of the multilayer interference stacks, but also to the specific surface morphology and texture of the coatings. These optical characteristics validate the spectral selectivity of the Al_xO_y–Pt–Al_xO_y interference-type multilayer stack for use in high temperature solar-thermal applications.     

Bulk crystalline BaPb34Bi14O3: A ceramic superconductor

The preparation conditions of the high T_C ceramic superconductor Ba(Pb,Bi)O₃ is correlated with the superconducting transition. Transition onsets of all materials are similar, but transition widths and transition completeness is strongly dependent on firing temperature. Only materials prepared over a narrow temperature range, resulting in a nearly ideal weight loss, have a complete and narrow transition.     

Electrostriction in Pb (Zn13Nb23)O3

The electrostriction in $\text{Pb (Zn}{}_{\mathrm{<mtext>1</mtext><mtext>3</mtext>}}\text{Nb}{}_{\mathrm{<mtext>2</mtext><mtext>3</mtext>}}\text{)}\text{O}{}_3$ crystals has been investigated using a strain gauge method. In the ferroelectric phase below 140 C, the strain vs the electric field shows a hysteresis, which is ascribed to the effect of ferroelectric domains. A quadratic relation holds between the strain x and the electric polarization P as x = QP² above about 170 C in the paraelectric phase. Values of the electrostrictive Q coefficients are determined from the measurements near 190 C, as Q₁₁ = 1.6·10^?2m⁴/C², Q₁₂ = ?0.86·10^?2m⁴/C², and Q₄₄ = 0.85·10^?2m⁴/C².     

Synthesis of a new perovskite Pb(Li14Nb34)O3

A high-pressure technique was adopted to obtain perovskite-type $\text{Pb(Li}{}_{\mathrm{<mtext>1</mtext><mtext>4</mtext>}}\text{Nb}{}_{\mathrm{<mtext>3</mtext><mtext>4</mtext>}}\text{)}\text{O}{}_3$. A new perovskite $\text{Pb(Li}{}_{\mathrm{<mtext>1</mtext><mtext>4</mtext>}}\text{Nb}{}_{\mathrm{<mtext>3</mtext><mtext>4</mtext>}}\text{)}\text{O}{}_3$ was characterized to have a cubic symmetry with $\text{a}{}_{\mathrm{<mtext>o</mtext>}}\text{= 4.069}\text{A}\text{?}$; Li and Nb ions in the B-site of perovskite lattice may be in a random arrangement.     

Magnetic,electrical and thermal studies on the V1−xMox02

The monoclinic-to-tetragonal structure transition of oxides V_1?xMo_x0₂ with $\text{0≤}\text{x}\text{≤0.20}$ has been studied by means of DTA, X-ray diffraction, magnetic susceptibility (powder samples) and electrical conductivity (single crystals) measurements within the temperature region 80 K to 400 K. A linear decrease of the transition temperature of 11 K per atom % Mo was observed. The magnetic susceptibility of the low temperature phase was found to be temperature independent paramagnetic for all preparations. Electrical conductivity measurements on the same phase showed crystals with $\text{x}\text{? 0.04}$ to be semiconducting, while a metallic behavior was observed in the region $\text{0.10 ?}\text{x}\text{? 0.14}$.     

n-PbTep+−Pb1−xSnxTe heterojunctions prepared by a modified hot wall technique

$\text{n-PbTe}\text{p}{}^{\mathrm{+}}\text{?}\text{Pb}{}_{\mathrm{1?x}}\text{Sn}{}_{\mathrm{x}}\text{Te}$ heterojunctions with a long wavelength spectral cutoff (λ_c ≈ 6 μm) were prepared using the double-channel hot wall technique. The electrical and photoelectrical properties of the heterojunctions at 77, 197 and 300 K were investigated. Detectors with R_oA equal to 170 Ω cm² and a quantum efficiency of 25–40% were obtained. Reasons for the shift of the long wavelength spectral cutoff of the heterojunctions towards shorter wavelengths are given.     

Optimization of AlxOy/Pt/AlxOy multilayer spectrally selective coatings for solar-thermal applications

Spectrally selective Al_xO_y/Pt/Al_xO_y multilayer absorber coatings were deposited onto corning 1737 glass, Si (111) and copper substrates using electron beam (e-beam) vacuum evaporator at room temperature. The employment of ellipsometric measurements and optical simulation was proposed as an effective method to optimize and deposit multilayer solar absorber coatings. The optical constants (n and k) measured using spectroscopic ellipsometry, showed that both Al_xO_y layers, which used in the coatings, were dielectric in nature and the Pt layer was semi-transparent. The optimized multilayer coatings exhibited high solar absorptance α ∼ 0.94 ± 0.01 and low thermal emittance ? ∼ 0.06 ± 0.01 at 82 °C. The Rutherford backscattering spectroscopy (RBS) data of Al_xO_y/Pt/Al_xO_y multilayer absorber indicated the Al_xO_y layers present in the coating were nearly stoichiometry. The scanning electron microscope analysis (SEM) result indicated that the average diameter and inter-particles distance of Pt grains were statistically about 146 ± 0.17 nm and 6-10 ± 0.2 nm respectively.     

Reactive plasma deposited SixCyHz films

Si_xC_yH_z films have been prepared at 200°C by reactive plasma deposition from SiH₄ and CH₄ diluted in helium in a tubular reactor. These films have a ratio s (equal to $\text{Si}\text{(}\text{Si+C}\text{))}$ ranging from 0.2 to 0.8, a refractive index ranging from 1.96 to 2.6 and an optical energy band gap in the range 2.7-2.2 eV. The total quantity of hydrogen in the film is 40% when s=0.5. Infrared analysis shows that these films have large fractions of homonuclear bonds and that this material is best described as a polymer. Mass spectrometric measurements of the gaseous products formed in the SiH₄-CH₄-He plasma have been performed and the results are related to the composition of the deposited layers.     

Core-current-enhanced domain-wall pinning in nanocrystalline Fe/sub 73.5/Cu/sub 1/Nb/sub 3/Si/sub 15.5/B/sub 7/ ribbon

We have studied the influence of surface fields H/sub p/ (generated by either direct or alternating core current) on soft magnetic properties of amorphous and nanocrystalline Fe/sub 73.5/Cu/sub 1/Nb/sub 3/Si/sub 15.5/B/sub 7/ ribbon. While in an amorphous ribbon the coercive field H/sub c/ decreases with H/sub p/, in the same optimally annealed ribbon (H/sub c/=1.3 A/m, M/sub m//spl ap/M/sub s/) H/sub c/ increases with H/sub p/ for all the explored types of H/sub p/ (static and dynamic with different phases with respect to that of the magnetizing field H). The unexpected increase of H/sub c/ in nanocrystalline ribbon is associated with the influence of H/sub p/ on the surface and main (inner) domain structure. Here, we develop a model that takes into account this influence and explains the experimental results.     

Interfacial microstructure of NiSix/HfO2/SiOx/Si gate stacks

Integration of NiSi_x based fully silicided metal gates with HfO₂ high-k gate dielectrics offers promise for further scaling of complementary metal-oxide- semiconductor devices. A combination of high resolution transmission electron microscopy and small probe electron energy loss spectroscopy (EELS) and energy dispersive X-ray analysis has been applied to study interfacial reactions in the undoped gate stack. NiSi was found to be polycrystalline with the grain size decreasing from top to bottom of NiSi_x film. Ni content varies near the NiSi/HfO_x interface whereby both Ni-rich and monosilicide phases were observed. Spatially non-uniform distribution of oxygen along NiSi_x/HfO₂ interface was observed by dark field Scanning Transmission Electron Microscopy and EELS. Interfacial roughness of NiSi_x/HfO_x was found higher than that of poly-Si/HfO₂, likely due to compositional non-uniformity of NiSi_x. No intermixing between Hf, Ni and Si beyond interfacial roughness was observed.